Simulation of entrainment of agglomerates from plate surfaces by shear flows
The entrainment process of agglomerates deposited on plate surfaces by shear flows was simulated using the three-dimensional modified discrete element method (mDEM) and influences of several factors on entrainment process were examined. In the case shear induced force is too weak, deposits are only...
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Veröffentlicht in: | Chemical engineering science 2009-04, Vol.64 (7), p.1455-1461 |
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creator | Iimura, Kenji Watanabe, Satoshi Suzuki, Michitaka Hirota, Mitsuaki Higashitani, Ko |
description | The entrainment process of agglomerates deposited on plate surfaces by shear flows was simulated using the three-dimensional modified discrete element method (mDEM) and influences of several factors on entrainment process were examined. In the case shear induced force is too weak, deposits are only deformed and particles are barely entrained, however, above some critical value particles are entrained by flows forming agglomerates. It was also clarified that the steric-bulky deposit undergoes the stronger hydrodynamic force and is easy to be entrained. There are two entrainment mechanisms corresponding to the parameter
A
s
/
A
which indicates the relative strength of adhesive force between particle and plate surface to that between particles. In case of large
A
s
/
A
where the adhesion between particle and plate surface is predominant, the number of entrained particles monotonically decreases as
A
s
/
A
increases due to the enhanced binding force. By contrast for small
A
s
/
A
, the number of entrained particles is not heavily dependent on
A
s
/
A
due to the mechanism in which the upstream side of deposit is lifted and the deposit is deformed extensively then large agglomerates are entrained. The boundary between those two entrainment mechanisms exists at
A
s
/
A
=
0.5
–
0.6
which is in good agreement with the theoretical prediction. |
doi_str_mv | 10.1016/j.ces.2008.10.070 |
format | Article |
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A
s
/
A
which indicates the relative strength of adhesive force between particle and plate surface to that between particles. In case of large
A
s
/
A
where the adhesion between particle and plate surface is predominant, the number of entrained particles monotonically decreases as
A
s
/
A
increases due to the enhanced binding force. By contrast for small
A
s
/
A
, the number of entrained particles is not heavily dependent on
A
s
/
A
due to the mechanism in which the upstream side of deposit is lifted and the deposit is deformed extensively then large agglomerates are entrained. The boundary between those two entrainment mechanisms exists at
A
s
/
A
=
0.5
–
0.6
which is in good agreement with the theoretical prediction.</description><identifier>ISSN: 0009-2509</identifier><identifier>EISSN: 1873-4405</identifier><identifier>DOI: 10.1016/j.ces.2008.10.070</identifier><identifier>CODEN: CESCAC</identifier><language>eng</language><publisher>Kidlington: Elsevier Ltd</publisher><subject>Agglomerate ; Applied sciences ; Chemical engineering ; DEM ; Deposit ; Detachment ; Discrete element method ; Entrainment ; Exact sciences and technology ; Plate surface ; Shear flow ; Simulation</subject><ispartof>Chemical engineering science, 2009-04, Vol.64 (7), p.1455-1461</ispartof><rights>2008 Elsevier Ltd</rights><rights>2009 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c424t-42a77ac30a1ca9edb6ccaafddc5f840a8ee7d00256878fe33723a530d2b327f33</citedby><cites>FETCH-LOGICAL-c424t-42a77ac30a1ca9edb6ccaafddc5f840a8ee7d00256878fe33723a530d2b327f33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.ces.2008.10.070$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,777,781,3537,27905,27906,45976</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=21343134$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Iimura, Kenji</creatorcontrib><creatorcontrib>Watanabe, Satoshi</creatorcontrib><creatorcontrib>Suzuki, Michitaka</creatorcontrib><creatorcontrib>Hirota, Mitsuaki</creatorcontrib><creatorcontrib>Higashitani, Ko</creatorcontrib><title>Simulation of entrainment of agglomerates from plate surfaces by shear flows</title><title>Chemical engineering science</title><description>The entrainment process of agglomerates deposited on plate surfaces by shear flows was simulated using the three-dimensional modified discrete element method (mDEM) and influences of several factors on entrainment process were examined. In the case shear induced force is too weak, deposits are only deformed and particles are barely entrained, however, above some critical value particles are entrained by flows forming agglomerates. It was also clarified that the steric-bulky deposit undergoes the stronger hydrodynamic force and is easy to be entrained. There are two entrainment mechanisms corresponding to the parameter
A
s
/
A
which indicates the relative strength of adhesive force between particle and plate surface to that between particles. In case of large
A
s
/
A
where the adhesion between particle and plate surface is predominant, the number of entrained particles monotonically decreases as
A
s
/
A
increases due to the enhanced binding force. By contrast for small
A
s
/
A
, the number of entrained particles is not heavily dependent on
A
s
/
A
due to the mechanism in which the upstream side of deposit is lifted and the deposit is deformed extensively then large agglomerates are entrained. The boundary between those two entrainment mechanisms exists at
A
s
/
A
=
0.5
–
0.6
which is in good agreement with the theoretical prediction.</description><subject>Agglomerate</subject><subject>Applied sciences</subject><subject>Chemical engineering</subject><subject>DEM</subject><subject>Deposit</subject><subject>Detachment</subject><subject>Discrete element method</subject><subject>Entrainment</subject><subject>Exact sciences and technology</subject><subject>Plate surface</subject><subject>Shear flow</subject><subject>Simulation</subject><issn>0009-2509</issn><issn>1873-4405</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNp9UE1LAzEQDaJgrf4Ab3vR29ZJstukeBLxCwoe1HOYZieasrupyVbpvzdLxaOHYXjD-2AeY-ccZhz4_Go9s5RmAkBnPAMFB2zCtZJlVUF9yCYAsChFDYtjdpLSOkOlOEzY8sV32xYHH_oiuIL6IaLvu7xHiO_vbego4kCpcDF0xSZzqUjb6DAHFqtdkT4IY-Ha8J1O2ZHDNtHZ756yt_u719vHcvn88HR7syxtJaqhrAQqhVYCcosLalZzaxFd09ja6QpQE6kGQNRzrbQjKZWQWEtoxEoK5aScssu97yaGzy2lwXQ-WWpb7Clsk5FSzyvNdSbyPdHGkFIkZzbRdxh3hoMZezNrk98wY2_jKfeWNRe_5pgsti5ib336EwouKznOlF3veZQ__fIUTbKeekuNj2QH0wT_T8oPUmaDrA</recordid><startdate>20090401</startdate><enddate>20090401</enddate><creator>Iimura, Kenji</creator><creator>Watanabe, Satoshi</creator><creator>Suzuki, Michitaka</creator><creator>Hirota, Mitsuaki</creator><creator>Higashitani, Ko</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>L7M</scope></search><sort><creationdate>20090401</creationdate><title>Simulation of entrainment of agglomerates from plate surfaces by shear flows</title><author>Iimura, Kenji ; Watanabe, Satoshi ; Suzuki, Michitaka ; Hirota, Mitsuaki ; Higashitani, Ko</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c424t-42a77ac30a1ca9edb6ccaafddc5f840a8ee7d00256878fe33723a530d2b327f33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Agglomerate</topic><topic>Applied sciences</topic><topic>Chemical engineering</topic><topic>DEM</topic><topic>Deposit</topic><topic>Detachment</topic><topic>Discrete element method</topic><topic>Entrainment</topic><topic>Exact sciences and technology</topic><topic>Plate surface</topic><topic>Shear flow</topic><topic>Simulation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Iimura, Kenji</creatorcontrib><creatorcontrib>Watanabe, Satoshi</creatorcontrib><creatorcontrib>Suzuki, Michitaka</creatorcontrib><creatorcontrib>Hirota, Mitsuaki</creatorcontrib><creatorcontrib>Higashitani, Ko</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Chemical engineering science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Iimura, Kenji</au><au>Watanabe, Satoshi</au><au>Suzuki, Michitaka</au><au>Hirota, Mitsuaki</au><au>Higashitani, Ko</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Simulation of entrainment of agglomerates from plate surfaces by shear flows</atitle><jtitle>Chemical engineering science</jtitle><date>2009-04-01</date><risdate>2009</risdate><volume>64</volume><issue>7</issue><spage>1455</spage><epage>1461</epage><pages>1455-1461</pages><issn>0009-2509</issn><eissn>1873-4405</eissn><coden>CESCAC</coden><abstract>The entrainment process of agglomerates deposited on plate surfaces by shear flows was simulated using the three-dimensional modified discrete element method (mDEM) and influences of several factors on entrainment process were examined. In the case shear induced force is too weak, deposits are only deformed and particles are barely entrained, however, above some critical value particles are entrained by flows forming agglomerates. It was also clarified that the steric-bulky deposit undergoes the stronger hydrodynamic force and is easy to be entrained. There are two entrainment mechanisms corresponding to the parameter
A
s
/
A
which indicates the relative strength of adhesive force between particle and plate surface to that between particles. In case of large
A
s
/
A
where the adhesion between particle and plate surface is predominant, the number of entrained particles monotonically decreases as
A
s
/
A
increases due to the enhanced binding force. By contrast for small
A
s
/
A
, the number of entrained particles is not heavily dependent on
A
s
/
A
due to the mechanism in which the upstream side of deposit is lifted and the deposit is deformed extensively then large agglomerates are entrained. The boundary between those two entrainment mechanisms exists at
A
s
/
A
=
0.5
–
0.6
which is in good agreement with the theoretical prediction.</abstract><cop>Kidlington</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.ces.2008.10.070</doi><tpages>7</tpages></addata></record> |
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language | eng |
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source | Elsevier ScienceDirect Journals |
subjects | Agglomerate Applied sciences Chemical engineering DEM Deposit Detachment Discrete element method Entrainment Exact sciences and technology Plate surface Shear flow Simulation |
title | Simulation of entrainment of agglomerates from plate surfaces by shear flows |
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